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Application of Experimental and Numerical Techniques to Microscale Devices

机译:实验和数值技术在微型器件中的应用

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摘要

Two of the areas that have become relevant recently are the areas of mixing in micro-scale devices, and manufacturing of functional nanoparticles. MicroPIV experiments were performed on two different mixers, one a wide microchannel with the surface grooves, in the laminar regime, and the other, a confined impinging jets reactor, in the laminar and turbulent regimes.In the wide microchannel with surface grooves, microPIV data were collected at the interface and the midplane at the Reynolds numbers of 0.08, 0.8, and 8. The experiments were performed on three internal angles of the chevrons, namely 135°, 90°, and 45°. The normalized transverse velocity generated in the midplane due to the presence of the grooves, is the strongest for the internal angle of 135°, and in that, the normalized transverse velocity is maximum at the Reynolds numbers of 0.08 and 0.8.MicroPIV experiments were performed in a confined impinging jets reactors at Reynolds numbers of 200, 1000, and 1500. The data was collected in the midplane, and turbulent statistics were further computed. The high velocity jets impinge along the centerline of the reactor. Upon impinging, part of the fluid turns towards the top wall and the majority of it turn towards the outlet. This high velocity impingement causes and unstable zone called the impingement zone, which moves about the centerline line, causing the jets to flap back and forth. Spatial correlations were computed to get an estimate of the size of the coherent structures. Large eddy simulation was performed on the CIJR for the Reynolds numbers of 1000 and 1500, using OpenFOAM. The Reynolds number is based on the inlet jet hydraulic diameter. Excellent agreement was found with the experimental and simulation data.Turbulent reactive mixing in a rectangular microscale confined impinging-jets reactor (CIJR)was investigated using the pH indicator phenolphthalein in this study for three di_erent jetReynolds numbers of 25, 1000 and 1500. Laminar flow regime was observed at Reynolds number of 25 whereas the flow was turbulent at Reynolds numbers of 1000 and 1500. An image processing technique was applied to instantaneous images to extract quantitative mixing data by identifying regions with pH ≥ 9.3 and regions with pH \u3c 9.3. The ensemble-averages were computed using these thresholded images to compare mixing performance between different Reynolds numbers. Finally, the spatial auto-correlation fields of the thresholded images fluctuations were evaluated, based on which large-scale turbulent structure were analyzed.
机译:最近变得重要的两个领域是微型设备中的混合领域和功能性纳米粒子的制造领域。 MicroPIV实验是在两种不同的混合器上进行的,一种是在层流状态下具有表面沟槽的宽微通道,另一种是在层流和湍流条件下是有限撞击射流反应器。在具有表面沟槽的宽微通道中,microPIV数据在界面和中平面处以雷诺数0.08、0.8和8收集了样品。实验是在人字形的三个内角(即135°,90°和45°)上进行的。由于凹槽的存在,在中平面产生的归一化横向速度在135°内角时最强,因为归一化横向速度在雷诺数为0.08和0.8时最大。在雷诺数分别为200、1000和1500的密闭撞击射流反应堆中进行数据收集。在中平面收集数据,并进一步计算湍流统计数据。高速射流沿反应堆中心线撞击。撞击时,一部分流体流向顶壁,而大部分流体流向出口。这种高速撞击会导致不稳定区域(称为撞击区域),该区域围绕中心线移动,从而导致射流来回摆动。计算空间相关性以获得对相干结构的大小的估计。使用OpenFOAM对CIJR进行了雷诺数为1000和1500的大涡模拟。雷诺数基于入口射流的液压直径。在实验和模拟数据中发现了很好的一致性。在这项研究中,使用pH指示剂酚酞研究了矩形微尺度密闭撞击式射流反应器(CIJR)中的湍流反应混合,分别研究了25、1000和1500的三种不同的雷诺数。层流在雷诺数为25的情况下观察到了这种状态,而在雷诺数为1000和1500的情况下则是湍流。将图像处理技术应用于即时图像,以通过识别pH≥9.3的区域和pH≥9.3的区域来提取定量混合数据。使用这些阈值图像计算总体平均值,以比较不同雷诺数之间的混合性能。最后,对阈值图像涨落的空间自相关域进行了评估,在此基础上分析了大规模湍流结构。

著录项

  • 作者

    Somashekar, Vishwanath;

  • 作者单位
  • 年度 2011
  • 总页数
  • 原文格式 PDF
  • 正文语种 en
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